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Inhomogeneous broadening of PAC spectra with Vn n zzn and η joint probability distribution functions

机译:用Vn n zzn和η联合概率分布函数对PAC光谱进行非均匀展宽

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摘要

The perturbed angular correlation (PAC) spectrum, G 2(t), is broadened by the presence of randomly distributed defects in crystals due to a distribution of electric field gradients (EFGs) experienced by probe nuclei. Heuristic approaches to fitting spectra that exhibit such inhomogeneous broadening (ihb) consider only the distribution of EFG magnitudes V zz , but the physical effect actually depends on the joint probability distribution function (pdf) of V zz and EFG asymmetry parameter η. The difficulty in determining the joint pdf leads us to more appropriate representations of the EFG coordinates, and to express the joint pdf as the product of two approximately independent pdfs describing each coordinate separately. We have pursued this case in detail using as an initial illustration of the method a simple point defect model with nuclear spin I = 5/2 in several cubic lattices, where G 2(t) is primarily induced by a defect trapped in the first neighbor shell of a probe and broadening is due to defects distributed at random outside the first neighbor shell. Effects such as lattice relaxation are ignored in this simple test of the method. The simplicity of our model is suitable for gaining insight into ihb with more than V zz alone. We simulate ihb in this simple case by averaging the net EFGs of 20,000 random defect arrangements, resulting in a broadened average G 2(t). The 20,000 random cases provide a distribution of EFG components which are first transformed to Czjzek coordinates and then further into the full Czjzek half plane by conformal mapping. The topology of this transformed space yields an approximately separable joint pdf for the EFG components. We then fit the nearly independent pdfs and reconstruct G 2(t) as a function of defect concentration. We report results for distributions of defects on simple cubic, face-centered cubic, and body-centered cubic lattices. The method explored here for analyzing ihb is applicable to more realistic cases.
机译:由于探针核所经历的电场梯度(EFG)的分布,晶体中随机分布的缺陷的存在使受扰的角度相关(PAC)光谱G 2(t)变宽。表现出这种不均匀展宽(ihb)的光谱的启发式方法仅考虑EFG幅度V zz的分布,但物理效果实际上取决于V zz和EFG不对称参数η的联合概率分布函数(pdf)。确定联合pdf的困难使我们获得了更合适的EFG坐标表示,并将联合pdf表示为分别描述每个坐标的两个近似独立pdf的乘积。我们以在几个立方晶格中具有核自旋I = 5/2的简单点缺陷模型作为该方法的初始说明来详细研究这种情况,其中G 2(t)主要是由捕获在第一个邻居中的缺陷引起的探针的壳变宽是由于缺陷在第一邻居壳外随机分布。在此方法的此简单测试中,诸如晶格弛豫的影响将被忽略。我们模型的简单性适合于仅凭V zz就可以深入了解ihb。在这种简单情况下,我们通过平均20,000个随机缺陷排列的净EFG来模拟ihb,从而导致平均G 2(t)变宽。 20,000个随机案例提供了EFG分量的分布,这些分量首先通过保形映射转换为Czjzek坐标,然后再转换为完整的Czjzek半平面。此变换空间的拓扑结构为EFG组件提供了近似可分离的联合pdf。然后,我们拟合几乎独立的pdf,并将G 2(t)重构为缺陷浓度的函数。我们报告在简单立方,面心立方和体心立方晶格上缺陷分布的结果。此处探讨的用于分析ihb的方法适用于更实际的情况。

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